2007
DOI: 10.1029/2007wr005934
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A general fractal model of flow and solute transport in randomly heterogeneous porous media

Abstract: [1] One of the challenges of hydrology is modeling flow and solute transport through media that are not uniformly porous. This paper proposes a general fractal model of flow and solute transport in randomly heterogeneous porous media. We describe the random field using fractional Levy motion (fLm), which more effectively represents a field with a high degree of variability. Understanding flow and solute transport in the fLm field expands the applicability of stochastic theory. Following the work of V. Di Feder… Show more

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Cited by 15 publications
(17 citation statements)
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References 36 publications
(62 reference statements)
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“…Observed multiscale behaviors of several subsurface fluid flow and transport variables in diverse geologic settings, at various sites and across a wide range of sampling domain scales have been found to be mutually consistent with a view of log permeability as a statistically isotropic or anisotropic self‐affine random field characterized by an α ‐order power variogram (semi‐structure function of order 2 when α = 2, width function when α < 2) γ α ( s ) = C 0 s αH (Neuman and Di Federico, ; Chen and Hsu, ; Neuman, ) where s is a scalar measure of distance (lag, defined in equivalent isotropic coordinates when the field is statistically anisotropic), C 0 being a constant, 0 < α ≤ 2 a Lévy index (Samorodnitsky and Taqqu, ) and 0 < H < 1 a Hurst exponent (Mandelbrot and Van Ness, ). The α ‐order power variogram scales as γ α ( rs ) = r αH γ α ( s ) for any r > 0.…”
Section: Introductionmentioning
confidence: 64%
“…Observed multiscale behaviors of several subsurface fluid flow and transport variables in diverse geologic settings, at various sites and across a wide range of sampling domain scales have been found to be mutually consistent with a view of log permeability as a statistically isotropic or anisotropic self‐affine random field characterized by an α ‐order power variogram (semi‐structure function of order 2 when α = 2, width function when α < 2) γ α ( s ) = C 0 s αH (Neuman and Di Federico, ; Chen and Hsu, ; Neuman, ) where s is a scalar measure of distance (lag, defined in equivalent isotropic coordinates when the field is statistically anisotropic), C 0 being a constant, 0 < α ≤ 2 a Lévy index (Samorodnitsky and Taqqu, ) and 0 < H < 1 a Hurst exponent (Mandelbrot and Van Ness, ). The α ‐order power variogram scales as γ α ( rs ) = r αH γ α ( s ) for any r > 0.…”
Section: Introductionmentioning
confidence: 64%
“…10 and 13 can be found in Chen (2007). If both a lower cutoff n l and an upper cutoff n u are considered, the truncated variogram becomes (Di Federico et al 1999):…”
Section: Two-point Statistics Of the Fractal Random Fieldmentioning
confidence: 99%
“…This was taken as an indication that the characteristic lengths of the modeled drainage areas are independently self‐affine in the one‐dimensional space Z of total channel length, rendering the network topologically anisotropic. Being self‐affine means forming a random function of the deterministic length measure Z (or, equivalently, a random field in Z ) and possessing a power (semi)variogram (or width function) γ () = A 0 αH where is a scalar measure of distance (lag) along the Z axis, α being a Levy index [ Chen and Hsu , 2007]. The power variogram scales as γ ( r ) = r αH γ () for any r > 0.…”
Section: Introductionmentioning
confidence: 99%